2 research outputs found
Synthesis, Crystal and Electronic Structure of the Quaternary Magnetic EuTAl<sub>4</sub>Si<sub>2</sub> (<i>T</i> = Rh and Ir) Compounds
Single crystals of the quaternary
europium compounds EuRhAl<sub>4</sub>Si<sub>2</sub> and EuIrAl<sub>4</sub>Si<sub>2</sub> were synthesized by using the Al–Si
binary eutectic as a flux. The structure of the two quaternary compounds
has been refined by single crystal X-ray diffraction. Both compounds
are stoichiometric and adopt an ordered derivative of the ternary
KCu<sub>4</sub>S<sub>3</sub> structure type (tetragonal <i>tP</i>8, <i>P</i>4/<i>mmm</i>). The two compounds reported
here represent the first example of a quaternary and truly stoichiometric
1:1:4:2 phase crystallizing with this structure type. In light of
our present results, the structure of the BaMg<sub>4</sub>Si<sub>3</sub> compound given in literature as representing a new prototype is
actually isotypic with the KCu<sub>4</sub>S<sub>3</sub> structure.
Local spin density approximation including the Hubbard <i>U</i> parameter (LSDA + <i>U</i>) calculations show that Eu
ions are in the divalent state, with a significant hybridization between
the Eu 5d, Rh (Ir) 4d (5d), Si 3p and Al 3p states. Magnetic susceptibility
measured along the [<i>001</i>] direction confirms the divalent
nature of the Eu ions in EuRhAl<sub>4</sub>Si<sub>2</sub> and EuIrAl<sub>4</sub>Si<sub>2</sub>, which order magnetically near ∼11 and
∼15 K, respectively
Synthesis and Characterization of ReS<sub>2</sub> and ReSe<sub>2</sub> Layered Chalcogenide Single Crystals
We report the synthesis of high-quality
single crystals of ReS<sub>2</sub> and ReSe<sub>2</sub> transition
metal dichalcogenides using
a modified Bridgman method that avoids the use of a halogen transport
agent. Comprehensive structural characterization using X-ray diffraction
and electron microscopy confirm a distorted triclinic 1<i>T</i>′ structure for both crystals and reveal a lack of Bernal
stacking in ReS<sub>2</sub>. Photoluminescence (PL) measurements on
ReS<sub>2</sub> show a layer-independent bandgap of 1.51 eV, with
increased PL intensity from thicker flakes, confirming interlayer
coupling to be negligible in this material. For ReSe<sub>2</sub>,
the bandgap is weakly layer-dependent and decreases from 1.31 eV for
thin layers to 1.29 eV in thick flakes. Both chalcogenides show feature-rich
Raman spectra whose excitation energy dependence was studied. The
lower background doping inherent to our crystal growth process results
in high field-effect mobility values of 79 and 0.8 cm<sup>2</sup>/(V
s) for ReS<sub>2</sub> and ReSe<sub>2</sub>, respectively, as extracted
from FET structures fabricated from exfoliated flakes. Our work shows
ReX<sub>2</sub> chalcogenides to be promising 2D materials candidates,
especially for optoelectronic devices, without the requirement of
having monolayer thin flakes to achieve a direct bandgap